358050 The electric field intensity at a point near and outside the surface of a charged conductor of any shape is \({E_1}\). The electric field intensity due to uniformly charged infinite thin plane sheet is \({E_2}\). The relation between \({E_1}\,{\rm{and}}\,{E_2}\) is

358051 Assertion :
\(E\) outside vicinity of a conductor depends only on the local charge density \(\sigma \) and it is independent of the other charges present anywhere on the conductor.
Reason :
\(E\) in outside vicinity of a conductor is given by \(\frac{\sigma }{{{\varepsilon _0}}}\).

358050 The electric field intensity at a point near and outside the surface of a charged conductor of any shape is \({E_1}\). The electric field intensity due to uniformly charged infinite thin plane sheet is \({E_2}\). The relation between \({E_1}\,{\rm{and}}\,{E_2}\) is

358051 Assertion :
\(E\) outside vicinity of a conductor depends only on the local charge density \(\sigma \) and it is independent of the other charges present anywhere on the conductor.
Reason :
\(E\) in outside vicinity of a conductor is given by \(\frac{\sigma }{{{\varepsilon _0}}}\).